Fractal behaviour of quantum paths in statistical physics
The path integral formalism is used to describe the statistical properties of an ideal gas of spinless particles. It is shown that the quantum paths exhibit the same properties in non-relativistic and relativistic domains provided the creation of new particles is avoided. Some quantities associat...
Збережено в:
Дата: | 2000 |
---|---|
Автор: | |
Формат: | Стаття |
Мова: | English |
Опубліковано: |
Інститут фізики конденсованих систем НАН України
2000
|
Назва видання: | Condensed Matter Physics |
Онлайн доступ: | http://dspace.nbuv.gov.ua/handle/123456789/121007 |
Теги: |
Додати тег
Немає тегів, Будьте першим, хто поставить тег для цього запису!
|
Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
Цитувати: | Fractal behaviour of quantum paths in statistical physics / J.P. Badiali // Condensed Matter Physics. — 2000. — Т. 3, № 3(23). — С. 545-558. — Бібліогр.: 19 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of UkraineРезюме: | The path integral formalism is used to describe the statistical properties of
an ideal gas of spinless particles. It is shown that the quantum paths exhibit
the same properties in non-relativistic and relativistic domains provided the
creation of new particles is avoided. Some quantities associated with the
paths are introduced, they have a simple meaning if the quantity βh , where
β is the reverse of the temperature, is considered as an ordinary time. The
relation between the velocity on the path and the momentum is not the
usual one, an extra term appears showing that the thermostat can not fix
the average value of this velocity although all the thermodynamic quantities
have their traditional values. The paths describe fluctuating trajectories on
which the particles do not follow the equation of motion. For time intervals
much shorter than βh we recover the properties of the Brownian motion.
The trajectories are located in space in a volume restricted by the Compton
wavelength for the short distances and the thermal de Broglie wavelength
for the largest ones. It is shown that the time-energy uncertainty is verified
on the quantum paths. This suggests that the density matrix obtained by
quantification of the classical canonical distribution function via the path integral formalism should not be totally identical to that obtained via the usual
route. Strong arguments are given showing that βh can be considered as
an ordinary time and not as a formal quantity having the same dimension
as time. This paper shows that for a time scale of 10 femtoseconds a totally new physics can be expected at room temperature. In addition it is
suggested that the ratio h/kB may play a decisive role in the foundation of
a covariant statistical physics. |
---|